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Welcome to GCSE Edexcel Science revision.

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Unit C P 11: Electromagnetic induction.

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A changing magnetic field through a coil or relative motion that cuts magnetic field lines can induce a potential difference.

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This is electromagnetic induction.

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Moving a magnet into or out of a coil changes the field through the coil.

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A sensitive voltmeter connected across the coil can detect an induced voltage.

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The voltmeter measures potential difference, with polarity set by connections.

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If the coil is part of a closed conducting circuit, the induced voltage drives a current.

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An open circuit can have induced voltage but no continuing current.

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A stationary magnet held within a stationary coil does not produce a continuing induced voltage because the field through the coil is not changing.

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Faster magnet movement, a stronger magnet or more coil turns can increase induced voltage when the other factors are fixed.

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Reverse the motion or reverse the magnet's poles to reverse the induced voltage direction.

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Reversing both can keep the direction unchanged.

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The field associated with the induced current opposes the original change.

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An approaching north pole induces a facing north pole that resists approach; a withdrawing north pole induces a facing south pole that resists separation.

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Both induced interactions resist the change that created them.

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This opposition means mechanical work is needed to maintain motion when electrical energy is transferred.

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Induction does not produce free energy.

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Connect a coil to a sensitive centre-zero voltmeter or data logger.

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Move a bar magnet in and out and record size and sign of voltage; compare with holding it still.

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Change one factor at a time: magnet speed, magnet strength or number of turns.

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Keep coil size, movement path, starting positions and other variables consistent.

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For fair comparisons, use repeatable movement and compare the same part of the movement or peak voltage.

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Repeat trials because hand movement gives varying speed.

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Investigate direction by reversing magnet motion or poles individually.

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Label which end of the coil is connected to the positive voltmeter terminal.

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A voltage pulse depends on the rate of field change, not simply how much magnetic material is sitting inside a coil.

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A transformer has a primary coil and a secondary coil linked by a magnetic core.

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The coils are electrically separate in the usual ideal model.

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A changing magnetic field transfers energy between them.

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Coils are magnetically coupled, not joined by an electrical wire.

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An alternating current in the primary creates a changing magnetic field in the core.

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The changing field through the secondary induces an alternating voltage.

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A secondary current flows if a load completes its circuit.

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An unloaded secondary can have voltage with little output power because there is little load current.

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A steady D C input does not provide the continuously changing field needed for normal transformer operation.

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Switching D C on or off can produce brief changes, not a sustained transformed output.

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A step-up transformer increases A C voltage; a step-down transformer decreases it.

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More secondary than primary turns gives step-up behaviour; fewer gives step-down behaviour.

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The core helps the magnetic field link both coils.

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Real transformers transfer some energy to the surroundings, including by heating, so their useful output power is less than their input power.

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For a transformer assumed one hundred percent efficient, input power equals output power.

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Use primary voltage times primary current equals secondary voltage times secondary current, with voltages in volts and currents in amperes.

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A primary of 230 volts and 2 amperes supplies 460 watts.

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If the ideal secondary is 23 volts, its current is 460 divided by 23 equals 20 amperes.

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Lower output voltage permits greater current at the same power.

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Increasing voltage reduces current for the same transferred power; reducing voltage increases current.

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A transformer cannot increase both output voltage and output current at unchanged input power.

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Rearrange the ideal equation to find a missing voltage or current.

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For example, secondary current equals primary voltage times primary current divided by secondary voltage.

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Check whether the question explicitly assumes an ideal transformer.

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If a real transformer has known efficiency, useful output power equals efficiency fraction times input power.

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Account for losses rather than claiming exact equality.

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The National Grid links generation and electricity transmission; local distribution networks deliver energy to consumers.

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Generation includes power stations and renewable sources.

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Step-up transformers raise voltage before long-distance transmission.

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For the same power, higher voltage means smaller current.

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Cable heating loss is power loss equals I squared times R.

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Reducing current greatly reduces heating losses for the same cable resistance, improving transmission efficiency.

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Halving current reduces I squared times R loss to a quarter.

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Step-down transformers reduce voltage for distribution and again near domestic users.

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UK domestic supply is approximately 230 volts A C; high transmission voltages would be unsuitable for direct household use.

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Illustrates the purpose of voltage changes rather than a universal list of grid voltages.

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Some transmission lines operate at hundreds of kilovolts, for example 400 kilovolts.

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Intermediate and generator voltages vary; the source's numbers are examples rather than one compulsory sequence.

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High-voltage equipment requires insulation, separation and controlled access.

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Lower domestic voltage still presents a serious electrical hazard.

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The grid transfers energy; it does not create it.

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Demand, generation and network operation must be managed, with some energy inevitably dissipated.

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That completes Electromagnetic induction.

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Revisit the notes and test yourself on the revision website.
